From d657f2a2edaa39f8f3545d6ac71e6a63b22faeba Mon Sep 17 00:00:00 2001
From: jps6 <jps6@cornell.edu>
Date: Tue, 10 Aug 2021 15:09:49 +0000
Subject: Update on Overleaf.

---
 ising_scaling.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

(limited to 'ising_scaling.tex')

diff --git a/ising_scaling.tex b/ising_scaling.tex
index c6dc29a..8bc17d7 100644
--- a/ising_scaling.tex
+++ b/ising_scaling.tex
@@ -148,7 +148,7 @@ models) in the literature \cite{Clement_2019_Respect}.
 In the low temperature phase, the free energy as a function of field has an essential singularity at zero field, which becomes a branch cut along the negative-$h$ axis when analytically continued to negative $h$ \cite{Langer_1967_Theory}. The origin can be schematically understood to arise from a
 singularity that exists in the complex free energy of the metastable phase of
 the model, suitably continued into the equilibrium phase. When the equilibrium
-Ising model with positive magnetization is subjected to a small negative
+Ising model with positive magnetization is subjehttps://www.overleaf.com/project/601afd459bf8018881b982a3cted to a small negative
 magnetic field, its equilibrium state instantly becomes one with a negative
 magnetization. However, under physical dynamics it takes time to arrive at this
 state, which happens after a fluctuation containing a sufficiently large
-- 
cgit v1.2.3-70-g09d2

